1985
DOI: 10.1364/ol.10.000490
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Energy band-gap dependence of two-photon absorption

Abstract: We present measurements of the two-photon absorption coefficients /2 of 10 different semiconductors having band-gap energies between 1.4 and 3.7 eV. We find that 12 varies as Eg-3 , as predicted by theory. In addition, the absolute values of 02 agree with theory, which includes the effect of nonparabolic bands, the average difference being less than 26%. This agreement permits confident predictions of two-photon absorption coefficients of other materials at other wavelengths.

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Cited by 319 publications
(192 citation statements)
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“…2(b)), which corresponds to Imχ (3) ∼ 10 −9 esu. This value is larger than that predicted from the gap-dependent scaling law derived for conventional semiconductors [12] by one order of magnitude, and is comparable to that of conventional 1D-structured materials. The scaling law [12] is inapplicable to Mott-insulators, in which the origin of the optical nonlinearity is the very large dipole coupling between nearly degenerate excited states of opposite parities.…”
mentioning
confidence: 48%
See 1 more Smart Citation
“…2(b)), which corresponds to Imχ (3) ∼ 10 −9 esu. This value is larger than that predicted from the gap-dependent scaling law derived for conventional semiconductors [12] by one order of magnitude, and is comparable to that of conventional 1D-structured materials. The scaling law [12] is inapplicable to Mott-insulators, in which the origin of the optical nonlinearity is the very large dipole coupling between nearly degenerate excited states of opposite parities.…”
mentioning
confidence: 48%
“…This value is larger than that predicted from the gap-dependent scaling law derived for conventional semiconductors [12] by one order of magnitude, and is comparable to that of conventional 1D-structured materials. The scaling law [12] is inapplicable to Mott-insulators, in which the origin of the optical nonlinearity is the very large dipole coupling between nearly degenerate excited states of opposite parities. The mechanism of optical nonlinearity here is related to that in the π-conjugated polymers, which are described within the one-band extended Hubbard model and in which also there occurs very large dipole coupling between the optical state and a two-photon state slightly higher in energy [13].…”
mentioning
confidence: 48%
“…The dielectric topcoating can be applied after MBE growth, which allows for additional flexibility in terms of finesse change of the structure. From a material point of view, SiO 2 and Si 3 N 4 are dielectric materials, and therefore exhibit negligible TPA compared to GaAs [50], which results in reduced IA. The nonlinear reflectivity measurements and corresponding extracted parameters are presented together with the measured damage thresholds in Figure 8a, and Table 3.…”
Section: Studied Structures and Obtained Resultsmentioning
confidence: 99%
“…35 The electron and hole wave functions ͓ e ͑r͒ and h ͑r͔͒ are determined by the multiplication of the radial wave function determined by Eqs. ͑2͒ and ͑3͒ with the spherical harmonics ͓i.e., R n,ᐉ ͑r͒Y ᐉ,m ͑ , ͔͒.…”
Section: Resultsmentioning
confidence: 99%